U.S. patent application number 11/695862 was filed with the patent office on 2007-10-18 for combined bragg grating wavelength interrogator and brillouin backscattering measuring instrument.
Invention is credited to TREVOR MacDOUGALL.
Application Number | 20070242262 11/695862 |
Document ID | / |
Family ID | 34522915 |
Filed Date | 2007-10-18 |
United States Patent
Application |
20070242262 |
Kind Code |
A1 |
MacDOUGALL; TREVOR |
October 18, 2007 |
COMBINED BRAGG GRATING WAVELENGTH INTERROGATOR AND BRILLOUIN
BACKSCATTERING MEASURING INSTRUMENT
Abstract
A method and apparatus sense attributes of reflected signals in
an optical sensing system. In one embodiment, a method for sensing
in an optical sensing system comprising an interrogator coupled to
a Bragg grating sensor by an optical cable includes the steps of
producing a first optical signal, coupling the first optical signal
to an optical cable, receiving a first reflected signal from a
Bragg grating sensor within the optical cable, resolving a
wavelength of first reflected signal, producing a second optical
signal, coupling the second optical signal to the optical cable,
receiving a second reflected signal caused by Brillouin
backscattering within the optical cable, and resolving a difference
in frequencies between the second optical signal and second
reflected signal. Embodiments of the method and apparatus are
particularly useful for sensing temperature and strain in hazardous
locations such as down hole gas and oil field applications and the
like.
Inventors: |
MacDOUGALL; TREVOR;
(Simsbury, CT) |
Correspondence
Address: |
PATTERSON & SHERIDAN, L.L.P.
3040 POST OAK BOULEVARD, SUITE 1500
HOUSTON
TX
77056
US
|
Family ID: |
34522915 |
Appl. No.: |
11/695862 |
Filed: |
April 3, 2007 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
|
|
10696766 |
Oct 29, 2003 |
7199869 |
|
|
11695862 |
Apr 3, 2007 |
|
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Current U.S.
Class: |
356/73.1 ;
374/E11.016 |
Current CPC
Class: |
E21B 47/07 20200501;
G01K 11/3206 20130101; G01D 5/35303 20130101 |
Class at
Publication: |
356/073.1 |
International
Class: |
G01N 21/00 20060101
G01N021/00 |
Claims
1. An apparatus for detecting Bragg grating reflected and
backscattered signals, comprising: a laser tunable over a
predefined wavelength range; an optical cable coupled to the laser;
a Bragg grating sensor coupled to the optical cable; a point
sensing circuit coupled to the optical cable for resolving a
wavelength of signals reflected from the Bragg grating sensor; and
a distributed sensing circuit coupled to the optical cable for
resolving a difference in frequency between a pulsed signal
provided by the laser and a backscattered signal, wherein the point
sensing circuit and the distributed sensing circuit are disposed
within a single interrogator.
2. The apparatus of claim 1, wherein the Bragg grating sensor
comprises a large diameter optical waveguide.
3. The apparatus of claim 1, wherein the Bragg grating sensor
comprises an optical fiber.
4. The apparatus of claim 1, wherein the point sensing circuit
comprises a wavemeter.
5. The apparatus of claim 1, wherein the distributed sensing
circuit comprises a frequency detector.
6. The apparatus of claim 1, wherein the laser is coupled to the
optical fiber via a pulse module configured to produce the pulsed
signal.
7. An apparatus for sensing reflected optical signals, comprising:
a Bragg grating sensor; an optical fiber coupled to the sensor; and
an interrogator coupled to the optical fiber and configured to
transmit and receive optical signals, wherein the received signals
are reflected from the Bragg grating sensor and backscattered along
a portion of the optical fiber, the received signals being
indicative of environmental conditions at the Bragg grating sensor
and along the portion of the optical fiber, and wherein the
interrogator is configured to distinguish between the received
signals reflected from the Bragg grating sensor and the received
signals backscattered along the portion of the optical fiber.
8. The apparatus of claim 7, wherein the Bragg grating sensor
comprises a large diameter optical waveguide.
9. The apparatus of claim 7, wherein the Bragg grating sensor
comprises an optical fiber.
10. The apparatus of claim 7, wherein the interrogator comprises a
tunable laser.
11. The apparatus of claim 7, wherein the interrogator comprises a
broadband light source coupled to a tunable filter.
12. The apparatus of claim 7, wherein the interrogator comprises a
pulse module configured to output the transmitted optical signals
as optical pulses.
13. The apparatus of claim 7, wherein the interrogator comprises an
optical switch configured to divert the received signals reflected
from the Bragg grating sensor to a first return path and the
received signals backscattered along the portion of the optical
fiber to a second return path.
14. The apparatus of claim 13, wherein the first return path is
coupled to a wavemeter.
15. The apparatus of claim 13, wherein the second return path is
coupled to a frequency detector.
16. The apparatus of claim 13, wherein the second return path
comprises at least one signal conditioning device.
17. The apparatus of claim 16, wherein the at least one signal
conditioning device is a Rayleigh filter.
18. The apparatus of claim 7, further comprising a controller
configured to process the received signals and/or control the
interrogator.
19. The apparatus of claim 18, wherein the controller is integrated
with the interrogator.
20. The apparatus of claim 18, wherein the controller is configured
to operate an optical switch for diverting the received signals
reflected from the Bragg grating sensor to a first return path and
the received signals backscattered along the portion of the optical
fiber to a second return path.
21. An apparatus for sensing reflected optical signals, comprising:
a Bragg grating sensor; an optical fiber coupled to the sensor; an
interrogator coupled to the optical fiber and configured to
transmit and receive optical signals, wherein the received signals
are reflected from the Bragg grating sensor and backscattered along
a portion of the optical fiber, the received signals being
indicative of a first environmental condition at the Bragg grating
sensor and a second environmental condition along the portion of
the optical fiber, and wherein the interrogator is configured to
distinguish between the received signals reflected from the Bragg
grating sensor and the received signals backscattered along the
portion of the optical fiber; and a controller configured to
receive the distinguished received signals from the interrogator
and to process a parameter indicative of the first environmental
condition from the received signals reflected from the Bragg
grating sensor and a parameter indicative of the second
environmental condition from the received signals backscattered
along the portion of the optical fiber.
22. The apparatus of claim 21, wherein the controller is integrated
with the interrogator.
Description
CROSS-REFERENCE TO RELATED APPLICATIONS
[0001] This application is a continuation of co-pending U.S. patent
application Ser. No. 10/696,766 filed Oct. 29, 2003, which is
herein incorporated by reference.
BACKGROUND OF THE INVENTION
[0002] 1. Field of the Invention
[0003] Embodiments of the invention generally relate to a method
and apparatus for detecting changes in a reflective signal in a
fiber optic sensing system.
[0004] 2. Background of the Related Art
[0005] For fiber optic sensing systems, specifically Bragg
grating-based systems, a dedicated opto-electronic instrument is
required to measure environmentally-induced changes in peak
wavelengths. If additional measurements, such as Brillouin-based
temperature and/or strain measurements are needed, additional
dedicated opto-electronic instrumentation is required. Systems
having dedicated instruments for sensing both Bragg grating and
Brillouin based measurements can be extremely costly and
complex.
[0006] Therefore, there is a need for an improved fiber optic
sensing system.
SUMMARY OF THE INVENTION
[0007] A method and apparatus for sensing using an optical fiber
are provided. In one embodiment, a method for sensing an attribute
(such as wavelength and/or frequency) of a reflected signal in an
optical fiber sensing system comprising an interrogator coupled to
a Bragg grating sensor by an optical cable includes the steps of
producing a first optical signal, coupling the first optical signal
to an optical cable, receiving a first reflected signal from a
Bragg grating sensor within the optical cable, resolving a
wavelength spectrum difference between the first optical signal and
first reflected signal, producing a second optical signal, coupling
the second optical signal to the optical cable, receiving a second
reflected signal caused by Brillouin backscattering within the
optical cable, and resolving a shift in wavelength spectrum between
the second optical signal and second reflected signal.
[0008] In another embodiment, an apparatus for sensing an attribute
in returning optical signals includes a Bragg grating sensor
coupled by an optical fiber to a light source and signal detection
circuit. The light source is suitable for producing optical signals
tunable over a range of wavelengths and is adapted to generate a
signal having sufficient intensity to produce Brillouin scattering
of the signal while propagating in the optical fiber. The signal
detection circuit includes a first sensing branch for detecting an
attribute of a signal reflected from the Bragg grating, a second
sensing branch for sensing an attribute of back-scattered signals
and an optical switch for diverting signals returning from the
optical fiber to the optical signal detection circuit selectively
between the first and second branches. Embodiments of the method
and apparatus are particularly useful for sensing temperature and
strain in hazardous locations such as down hole gas and oil field
applications and the like.
BRIEF DESCRIPTION OF THE DRAWINGS
[0009] A more particular description of the invention, briefly
summarized above, may be had by reference to the embodiments
thereof that are illustrated in the appended drawings. It is to be
noted, however, that the appended drawings illustrate only typical
embodiments of this invention and are therefore not to be
considered limiting of its scope, for the invention may admit to
other equally effective embodiments. So that the manner in which
the above-recited embodiments of the invention are obtained and can
be understood in detail, a more particular description of the
invention, briefly summarized above, may be had by reference to the
embodiments thereof which are illustrated in the appended drawings.
It is to be noted, however, that the appended drawings illustrate
only typical embodiments of this invention and are, therefore, not
to be considered limiting of its scope, for the invention may admit
to other equally effective embodiments.
[0010] FIG. 1 is a system-level view of a fiber optic sensing
system suitable for use in oil or gas well applications;
[0011] FIG. 2 is one embodiment of a sensor of the system of FIG.
1;
[0012] FIG. 3 is a schematic of one embodiment of an interrogator
of FIG. 1; and
[0013] FIGS. 4A-C are a flow diagram of one embodiment of a method
for sensing wavelength shifts in returning optical signals.
[0014] To facilitate understanding, identical reference numerals
have been used, wherever possible, to designate identical elements
that are common to the figures.
DETAILED DESCRIPTION
[0015] FIG. 1 is a simplified schematic of an oil or gas well 110
having an optical fiber sensing system 100 adapted to sense
environmental conditions within the well 110 using a method and
apparatus of the present invention. The well 110 includes a main
bore 112 extending from a wellhead 114. The sensing system 100
utilizes both Bragg grating reflections and non-linear induced back
scatter signals to resolve environmental conditions along the
sensing path. In one embodiment, wavelengths and/or frequency of
reflected signals are indicative of temperature and strain
information of the environmental conditions within the well
110.
[0016] The sensing system 100 includes an interrogator 160 coupled
by an optic cable 162 to at least one sensor 164. The sensor 164
may be a single point sensor or other suitable Bragg grating
sensor. One sensor 164 that may be utilized is available from
Weatherford, Inc., located in Houston, Tex. Another example of a
sensor 164 that may be utilized is described in U.S. Pat. No.
6,422,084, entitled "Bragg Grating Pressure Sensor", issued Jul.
23, 2002 to Fernald et al.; and U.S. Pat. No. 6,452,667, entitled
"Pressure Isolated Bragg Grating Temperature Sensor", issued Sep.
17, 2002, to Fernald et al., all of which are hereby incorporated
by reference in their entireties.
[0017] FIG. 2 depicts one embodiment of the sensor 164. The sensor
164 includes a large diameter optical waveguide 210, has at least
one core 212 surrounded by a cladding 214, similar to that
disclosed in U.S. Pat. No. 6,363,089 entitled "Large Diameter
Optical Waveguide, Grating, and Laser", which is incorporated
herein by reference. The waveguide 210 comprises silica glass
(SiO.sub.2) based material having the appropriate dopants, as is
known, to allow light 215 to propagate in either direction along
the core 212 and/or within the waveguide 210. The core 212 has an
outer dimension d1 and the waveguide 210 has an outer dimension d2.
Other materials for the optical waveguide 210 may be used if
desired. For example, the waveguide 210 may be made of any glass,
e.g., silica, phosphate glass, or other glasses; or solely
plastic.
[0018] In one embodiment, the outer dimension d2 of the cladding
214 is at least about 0.3 mm and outer dimension d1 of the core 212
such that it propagates only a few spatial modes (e.g., less than
about 6). For example for single spatial mode propagation, the core
212 has a substantially circular transverse cross-sectional shape
with a diameter d1 less than about 12.5 microns, depending on the
wavelength of light. The invention will also work with larger or
non-circular cores that propagate a few (less than about 6) spatial
modes, in one or more transverse directions. The outer diameter d2
of the cladding 214 and the length L have values that will resist
buckling when the waveguide 210 is placed in axial compression as
indicated by the arrows 218.
[0019] The waveguide 210 may be ground or etched to provide tapered
(or beveled or angled) outer corners or edges 224 (shown in
phantom) to provide a seat for the waveguide 210 to mate with
another part (not shown) and/or to adjust the force angles on the
waveguide 210, or for other reasons. The angle of the beveled
corners 224 is set to achieve the desired function. Further, the
waveguide may be etched or ground to provide nubs for an attachment
of a pigtail assembly to the waveguide. Further, the size of the
waveguide 210 has inherent mechanical rigidity that improves
packaging options and reduces bend losses.
[0020] The waveguide has a Bragg grating 216 impressed (or embedded
or imprinted) therein. The Bragg grating 216, as is known, is a
periodic or aperiodic variation in the effective refractive index
and/or effective optical absorption coefficient of an optical
waveguide. The grating 216 may be in the core 212 and/or in the
cladding 214 (shown in the core 212 in FIG. 2). Any
wavelength-tunable grating or reflective element embedded, etched,
imprinted, or otherwise formed in the waveguide 210 may be used if
desired. The waveguide 210 may be photosensitive if a grating 216
are to be written into the waveguide 210. As used herein, the term
"grating" means any of such reflective elements. Further, the
reflective element (or grating) 16 may be used in reflection and/or
transmission of light. Light 215 incident on the grating 216
reflects a portion thereof as indicated by a line 236 having a
predetermined wavelength band of light, and passes the remaining
wavelengths of the incident light 215 (within a predetermined
wavelength range), as indicated by a line 238 (as is known).
[0021] The grating 216 has a grating length Lg, which is determined
based on the application, may be any desired length. A typical
grating 216 has a grating length Lg in the range of about 3-40 mm.
Other sizes or ranges may be used if desired. The length Lg of the
grating 216 may be shorter than or substantially the same length as
the length L of the waveguide 210. Also, the core 212 need not be
located in the center of the waveguide 210 but may be located
anywhere in the waveguide 210.
[0022] Accordingly, we have found that the present invention also
reduces coupling between the core and cladding modes due to the
increased end cross-sectional area between the core and cladding of
the waveguide. Thus, a grating 216 written in the core 212 of the
waveguide 210 exhibits less optical transmission loss and exhibits
a cleaner optical profile than a conventional fiber grating because
the large cladding region dissipates coupled cladding modes,
thereby reducing the coupling of the core 212 to the cladding 214
modes. In general, the greater the difference in cross-sectional
area between the core 212 and the cladding 214 the smaller the mode
field overlap and the lower the coupling to the cladding modes. The
thickness of the cladding 214 between the cladding outer diameter
and the core outer diameter may be set to optimize this effect.
Other diameters of the core 212 and waveguide 210 may be used if
desired such that the cladding modes are reduced to the desired
levels.
[0023] The waveguide 210 may have end cross-sectional shapes other
than circular, such as square, rectangular, elliptical, clam-shell,
octagonal, multi-sided, or any other desired shapes, discussed more
hereinafter. Also, the waveguide may resemble a short "block" type
or a longer "cane" type geometry, depending on the length of the
waveguide and outer dimension of the waveguide.
[0024] The side cross-section of the outer surface of the waveguide
210 may have a varying geometry, depending on the application. For
example, the waveguide 210 may have a "dogbone" shape having a
narrow central section and larger outer sections. The dogbone shape
may be used to provide increased sensitivity in converting axial
force to length change .DELTA.L and/or wavelength shift
.DELTA..lamda. of the grating 216 and may be achieved by etching,
grinding, machining, heating & stretching, or other known
techniques.
[0025] The dimensions and geometries for any of the embodiments
described herein are merely for illustrative purposes and, as such,
any other dimensions may be used if desired, depending on the
application, size, performance, manufacturing requirements, or
other factors, in view of the teachings herein.
[0026] The optical waveguide 210 may be formed by heating,
collapsing and fusing a glass capillary tube to a fiber (not shown)
by a laser, filament, flame, etc., as is described U.S. Pat. No.
6,519,388, entitled "Tube-Encased Fiber Grating," which is
incorporated herein by reference. Alternatively, other techniques
may be used to fuse the fiber to the tube, such as using a high
temperature glass solder, e.g., a silica solder (powder or solid),
such that the fiber, the tube and the solder all become fused to
each other, or using laser welding/fusing or other fusing
techniques.
[0027] The Bragg grating may be written in the fiber before or
after the capillary tube is encased around and fused to the fiber,
such as is discussed in the above referenced U.S. Pat. No.
6,519,388. If the grating is written in the fiber after the tube is
encased around the grating, the grating may be written through the
tube into the fiber by any desired technique, such as is described
in U.S. Pat. No. 6,298,184, entitled "Method and Apparatus For
Forming A Tube-Encased Bragg Grating", filed Dec. 4, 1998, which is
incorporated herein by reference.
[0028] Returning to FIG. 1, the optic cable 162 generally includes
one or more optical fibers suitable for transmitting optic signals
between the interrogator 160 and the sensor 164. Examples of
suitable optic cables are described in U.S. Pat. No. 6,404,961,
issued Jun. 11, 2002 to Bonja et al., and U.S. patent application
Ser. No. 10/422,396, filed Apr. 24, 2003 by Dowd et al., both of
which are hereby incorporated by reference in their entireties.
Suitable cables are also available from Weatherford, Inc.
[0029] In the embodiment depicted in FIG. 1, the optic cable 162
includes one or more single-mode optical fibers 122 disposed in a
protective sleeve 124 suitable to protect the optical fibers 122 in
a down hole well environment. In some applications, the optical
cable 162 may extend up to and exceed 12 kilometers through main
bore 112 and/or at least one of the secondary bores (not shown)
that may branch out from the main bore 112 within the well 110.
[0030] In one embodiment, the sleeve 124 includes an inner tube 126
seam welded around the one or more optical fibers 122, a spacer 128
and an outer metal tube 130. The inner tube 126 may be filled with
a material 132, for example a getter gel, utilized to support the
one or more optical fibers 122 in the inner tube 126. The outer
metal tube 130 is welded around the spacer 128 that is disposed
between the inner and outer tubes 126, 130. A barrier material (not
shown) having low hydrogen permeability may be disposed on at least
one of the tubes 126, 130.
[0031] The interrogator 160 is configured to transmit and receive
optical signals through the optic cable 162. The interrogator 160
is suitable for interrogating both Bragg grating based sensors and
non-linear induced backscatter signals to provide a metric
indicative of the wavelength and/or frequency of reflected signals
that are indicative environmental conditions within the well, for
example, temperature and strain. In addition, other environmental
conditions may be detected by the optical Bragg grating based
sensor such as pressure, seismic disturbances, chemicals, etc., as
is well known in the art. It is also contemplated within the scope
of present invention that multiple optical Bragg grating based
sensors positioned along the cable and multiplexed as is known in
the art.
[0032] FIG. 3 depicts one embodiment of the interrogator 160. The
interrogator 160 includes a signal generator 302, a pulse module
304, a frequency detector 316 and an optical wavemeter 318. A
controller 340 is coupled to the interrogator 160 for processing
information provided by the frequency detector 316 and the optical
wavemeter 318. Alternatively, the controller 340 may be an integral
part of the interrogator 160. The controller 340 may also manages
signal generation, collection and interpretation of data, and the
general operation of the sensing system 100.
[0033] The controller 340 includes a central processing unit (CPU)
342, support circuits 344 and memory 346. The CPU 342 may be one of
any form of general purpose computer processor that can be used in
an industrial setting configured to interface with the interrogator
160. The memory 346 is coupled to the CPU 342. The memory 346, or
computer-readable medium, may be one or more of readily available
memory such as random access memory (RAM), read only memory (ROM),
floppy disk, hard disk, or any other form of digital storage, local
or remote. The support circuits 344 are coupled to the CPU 342 for
supporting the processor in a conventional manner. These circuits
include cache, power supplies, clock circuits, input/output
circuitry and subsystems, and the like.
[0034] The signal generator 302 is coupled to a first tap 322. The
first tap 322 selectively directs portions of an output of the
signal generator 302 to the pulse module 304 and the wavemeter 318.
The percentage of the signal diverted by the first tap 322 may be
selected based on the depth of the sensor 164 within the well,
among other factors.
[0035] A second tap 324 is disposed between the first tap 322 and
the wavemeter 318 to divert a portion of the signal passing
therebetween to the frequency detector 316. The pulse module 304 is
coupled to the optic cable 162 such that an output signal (shown by
arrow 306) from the interrogator 160 may be sent through the cable
162 to the sensor 164 (shown in FIG. 1).
[0036] An optical switch 320 is disposed in the interrogator 160
for selectively diverting reflected return signals (shown by arrow
308) between a first return path 310 and a second return path 312.
The first return path 310 directs the return signals 306 reflected
from the sensor 164 to the wavemeter 318. The second return path
312 directs the Brillouin backscattered return signals 306 to the
frequency detector 316.
[0037] The signal generator 302 is configured to produce an optical
signal into the optical fiber 122. The signal generator 302 may
produce a single polarized optical signal and may have an output
adjustable in power and of intensity sufficient to produce
Brillouin scattering of the signal as the signal propagates through
the optical fiber 122 down the well 110. In one embodiment, the
intensity of the signal is at least about 100 microwatts. The
signal generator 102 is configured to produce an output signal
tunable at least between wavelengths reflected and transmissive to
the sensor 164 (e.g., not in the sensor band). In one embodiment,
the signal generator 302 is a semiconductor laser having an output
signal tunable between at least about 3 to about 6 kilometers over
the reflected band of the sensor 164. Alternatively, the signal
generator 302 may be a broadband light source coupled with a
tunable filter.
[0038] The pulse module 304 may be set to a first state that allows
the output signal of the signal generator to pass directly
therethrough. The pulse module 304 may be set to a second state
that pulses the output signal through the optical cable 162. The
pulse rate is generally selected to allow individual pulses to be
reflected without interference from subsequently launched
signals.
[0039] The second return path 312 may include one or more signal
conditioning devices suitable for enhancing the performance of the
frequency detector 316 in analyzing Brillouin backscattered return
signals. In one embodiment, the conditioning device disposed on the
second return path 312 between the switch 320 and the frequency
detector 316 is a Rayleigh filter 314. The Rayleigh filter 314
conditions the returning signals and improve system performance by
removing extraneous portions of the reflected signal not required
for the analysis of the conditions along the sensing path.
[0040] The wavemeter 318 is a high resolution wavelength detector
and is configured to receive reflected signals returning through
the optical fiber 122 of the cable 162 and launched signals tapped
from the signal generator 302. The wavemeter 318 is also configured
to determine the amplitude of the optical signals. The wavemeter
318 may include one or more photodiodes for converting the optical
signal to a digital signal. The wavemeter 318 provides the
controller 340 with a metric indicative of the wavelength (and/or
frequency) of the launched and reflected signals.
[0041] The frequency detector 316 is a high resolution frequency
detector and is configured to receive backscattered signals
returning through the optical fiber 122 of the cable 162 and
launched signals tapped from the signal generator 302. The
frequency detector 316 resolves a difference in frequency between
the launched and reflected signals. A metric indicative of the
difference in frequency is provided to the controller 340 which is
indicative of environmental conditions at the portion of the fiber
from which the backscattered signal was reflected.
[0042] A sensing method 400, described below with reference to the
flow diagrams illustrated in FIGS. 4A-C, is generally stored in the
memory 346 of the controller 340, typically as a software routine.
The software routine may also be stored and/or executed by a second
CPU (not shown) that is remotely located from the hardware being
controlled by the CPU 342. When the routine is executed by the CPU
342, the controller 340 provides instructions to the signal
generator 302 and receives data from the frequency detector 316 and
wavemeter 318, from which an attribute, such as wavelength and/or
frequency of returning optical signals may be resolved. In one mode
of operation, the resolved attributes may be indicative of
temperature and/or strain at one or more predefined positions along
the optical fiber 122 that corresponds depth and/or location within
the well 110.
[0043] FIGS. 4A-C are flow diagrams of one embodiment of the method
400 for resolving a measure of one or more environmental conditions
from attributes of returning optical signals. The method 400 begins
by performing a point sensing step 420 and may be followed by a
distributed sensing step 460. The point sensing step 420 is mainly
utilized to resolve a measure of one or more environmental
conditions at the sensor 164.
[0044] The point sensing step 420 begins at step 422 by producing a
series of output signals 306 from the signal generator 302 through
a band of wavelengths from the interrogator 160 to the sensor 164.
In one embodiment, the output signals 306 may be produced by
scanning a laser through a predefined range of output
wavelengths.
[0045] At step 424, the tap 322 selectively diverts a portion of
the signal 306 produced by the interrogator 160 to the wavemeter
318 through the tap 324. At step 426, the wavemeter 318 records
and/or characterizes the amplitude versus time of the reflected
signal 308 returning via the first return path 310. At step 330, a
peak wavelength of the reflected signal is resolved by determining
the time corresponding to the peak amplitude of the reflected
signal, from which the wavelength may be derived using the
time/wavelength relationship characterized from the launched
signal. At step 432, the wavelength information of the reflected
signal 308 is correlated to environmental parameters (for example,
strain and/or temperature) at the sensor 164.
[0046] The distributed sensing step 460 begins at step 462 where
the signal generator 302 produces a signal tuned to a wavelength
not in the band of the grating (e.g., sensor 164). The signal
generally has sufficient power to induce Brillouin scattering as
the signal propagates through the optical cable 162. At step 464,
the taps 322, 324 selectively diverts a portion of the produced
signal 306 to the frequency detector 316. At step 466, the
remainder of the signal (e.g., the portion not diverted at step
464) is pulsed by the pulse module 304. The pulse module 304 is set
to pulse the output signal 306 traveling down the optic cable 162
toward the sensor 164.
[0047] At step 468, the frequency detector 316 records and/or
characterizes the frequency (and/or wavelength) of the output
signal 306. At step 470, the frequency detector 3126 records and/or
characterizes the frequency (and/or wavelength) of the
backscattered (reflected) signal 308 returning to the frequency
detector 316 via the second return path 320. At step 372, a shift
in difference in the frequencies (and/or wavelengths) between the
output signal 306 and the backscattered signal 308 is resolved
which indicates a change in the environmental parameters along the
distributed length of the optical cable 162. The shift in the
backscattered signal 308 is indicative of changes in environmental
conditions along the sensing string (e.g., the length of the
optical cable 162). Analysis of the change in wavelength of the
backscattered signal 308 can be resolved, for example, by the
controller 340, to provide distributed strain and temperature
information over the length of the optical cable 162, which
corresponds to distinct locations along the main bore 112 of the
well 110.
[0048] Thus, a method and apparatus has been presented for
accurately sensing the attributes in both Bragg grating and
Brillouin backscattered optical signals. The invention
advantageously minimizes the amount of measurement equipment
required to sense both types of reflected signals, thereby reducing
the cost of and complexity of measurement equipment. The invention
is particularly suitable for use in hazardous locations, such as
oil and gas well applications, where changes in signal wavelengths
are indicative of environmental changes within the well, such as
changes in temperature and strain.
[0049] Although several embodiments which incorporate the teachings
of the present invention have been shown and described in detail,
those skilled in the art can readily devise many other varied
embodiments that still incorporate these teachings.
* * * * *